1. | segment \(1\) | 2. | segment \(2\) |
3. | segment \(3\) | 4. | segment \(4\) |
1. | \(\dfrac{\mu_{0} I}{6}\) | 2. | \(\dfrac{2 \mu_{0} I}{6}\) |
3. | \(\dfrac{4\mu_{0} I}{6}\) | 4. | \(\dfrac{5\mu_{0} I}{6}\) |
1. | field is the same every where around the conductor. |
2. | field is directly proportional to the square of the current flowing in the conductor. |
3. | field obeys the inverse square law of distance. |
4. | magnetic field strength was maximum on the axis of the current conductor. |
1. | \(16K\) | 2. | \(8K\) |
3. | \(4K\) | 4. | \(K\) |
1. | \(\left({{i}_{0}\mathit{\pi}{R}_{0}^{2}}\right)\sqrt{2} \) | 2. | zero |
3. | \({i}_{0}\times{2}\mathit{\pi}{R}_{0}^{2} \) | 4. | \({i}_{0}\left({{4}\mathit{\pi}{R}_{0}}\right) \) |
1. | \(\dfrac{\mu_0i}{4r}\) |
2. | \(\dfrac{\mu_0i}{4r}+\dfrac{\mu_0i}{2\pi r}\) |
3. | \(\dfrac{\mu_0i}{4r}+\dfrac{\mu_0i}{4\pi r}\) |
4. | \(\left[\left(\dfrac{\mu_0i}{4r}\right)^2+\left(\dfrac{\mu_0i}{4\pi r}\right)^2\right]^{\frac12} \) |
1. | \(6.28 \times 10^{-4} ~\text{T} \) | 2. | \(6.28 \times 10^{-2}~\text{T}\) |
3. | \(12.56 \times 10^{-2}~\text{T}\) | 4. | \(12.56 \times 10^{-4} ~\text{T}\) |
1. | A linearly decreasing function of distance upto the boundary of the wire and then a linearly increasing one for the outside region. |
2. | Uniform and remains constant for both regions. |
3. | A linearly increasing function of distance upto the boundary of the wire and then a linearly decreasing one for the outside region. |
4. | A linearly increasing function of distance \(r\) upto the boundary of the wire and then decreasing one with \(1/r\) dependence for the outside region. |
The ratio of the radii of two circular coils is \(1:2.\) The ratio of currents in the respective coils such that the same magnetic moment is produced at the centre of each coil is:
1. | \(4:1\) | 2. | \(2:1\) |
3. | \(1:2\) | 4. | \(1:4\) |